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  • Balter, Peter A.  (16)
  • Court, Laurence E.  (16)
  • 1
    In: Computerized Medical Imaging and Graphics, Elsevier BV, Vol. 40 ( 2015-03), p. 30-38
    Type of Medium: Online Resource
    ISSN: 0895-6111
    Language: English
    Publisher: Elsevier BV
    Publication Date: 2015
    detail.hit.zdb_id: 2004841-5
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  • 2
    In: Practical Radiation Oncology, Elsevier BV, Vol. 12, No. 4 ( 2022-07), p. e344-e353
    Type of Medium: Online Resource
    ISSN: 1879-8500
    Language: English
    Publisher: Elsevier BV
    Publication Date: 2022
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  • 3
    In: Advances in Radiation Oncology, Elsevier BV, Vol. 6, No. 4 ( 2021-07), p. 100683-
    Type of Medium: Online Resource
    ISSN: 2452-1094
    Language: English
    Publisher: Elsevier BV
    Publication Date: 2021
    detail.hit.zdb_id: 2847724-8
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  • 4
    In: Journal of Global Oncology, American Society of Clinical Oncology (ASCO), , No. 4 ( 2018-12), p. 1-11
    Abstract: We assessed automated contouring of normal structures for patients with head-and-neck cancer (HNC) using a multiatlas deformable-image-registration algorithm to better provide a fully automated radiation treatment planning solution for low- and middle-income countries, provide quantitative analysis, and determine acceptability worldwide. Methods Autocontours of eight normal structures (brain, brainstem, cochleae, eyes, lungs, mandible, parotid glands, and spinal cord) from 128 patients with HNC were retrospectively scored by a dedicated HNC radiation oncologist. Contours from a 10-patient subset were evaluated by five additional radiation oncologists from international partner institutions, and interphysician variability was assessed. Quantitative agreement of autocontours with independently physician-drawn structures was assessed using the Dice similarity coefficient and mean surface and Hausdorff distances. Automated contouring was then implemented clinically and has been used for 166 patients, and contours were quantitatively compared with the physician-edited autocontours using the same metrics. Results Retrospectively, 87% of normal structure contours were rated as acceptable for use in dose-volume-histogram–based planning without edit. Upon clinical implementation, 50% of contours were not edited for use in treatment planning. The mean (± standard deviation) Dice similarity coefficient of autocontours compared with physician-edited autocontours for parotid glands (0.92 ± 0.10), brainstem (0.95 ± 0.09), and spinal cord (0.92 ± 0.12) indicate that only minor edits were performed. The average mean surface and Hausdorff distances for all structures were less than 0.15 mm and 1.8 mm, respectively. Conclusion Automated contouring of normal structures generates reliable contours that require only minimal editing, as judged by retrospective ratings from multiple international centers and clinical integration. Autocontours are acceptable for treatment planning with no or, at most, minor edits, suggesting that automated contouring is feasible for clinical use and in the ongoing development of automated radiation treatment planning algorithms.
    Type of Medium: Online Resource
    ISSN: 2378-9506
    Language: English
    Publisher: American Society of Clinical Oncology (ASCO)
    Publication Date: 2018
    detail.hit.zdb_id: 3018917-2
    detail.hit.zdb_id: 2840981-4
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  • 5
    In: Medical Physics, Wiley, Vol. 47, No. 11 ( 2020-11), p. 5592-5608
    Abstract: The purpose of this work was to evaluate the performance of X‐Net, a multiview deep learning architecture, to automatically label vertebral levels (S2‐C1) in palliative radiotherapy simulation CT scans. Methods For each patient CT scan, our automated approach 1) segmented spinal canal using a convolutional‐neural network (CNN), 2) formed sagittal and coronal intensity projection pairs, 3) labeled vertebral levels with X‐Net, and 4) detected irregular intervertebral spacing using an analytic methodology. The spinal canal CNN was trained via fivefold cross validation using 1,966 simulation CT scans and evaluated on 330 CT scans. After labeling vertebral levels (S2‐C1) in 897 palliative radiotherapy simulation CT scans, a volume of interest surrounding the spinal canal in each patient's CT scan was converted into sagittal and coronal intensity projection image pairs. Then, intensity projection image pairs were augmented and used to train X‐Net to automatically label vertebral levels using fivefold cross validation ( n  = 803). Prior to testing upon the final test set ( n  = 94), CT scans of patients with anatomical abnormalities, surgical implants, or other atypical features from the final test set were placed in an outlier group ( n  = 20), whereas those without these features were placed in a normative group ( n  = 74). The performance of X‐Net, X‐Net Ensemble, and another leading vertebral labeling architecture (Btrfly Net) was evaluated on both groups using identification rate, localization error, and other metrics. The performance of our approach was also evaluated on the MICCAI 2014 test dataset ( n  = 60). Finally, a method to detect irregular intervertebral spacing was created based on the rate of change in spacing between predicted vertebral body locations and was also evaluated using the final test set. Receiver operating characteristic analysis was used to investigate the performance of the method to detect irregular intervertebral spacing. Results The spinal canal architecture yielded centroid coordinates spanning S2‐C1 with submillimeter accuracy (mean ± standard deviation, 0.399 ± 0.299 mm; n  = 330 patients) and was robust in the localization of spinal canal centroid to surgical implants and widespread metastases. Cross‐validation testing of X‐Net for vertebral labeling revealed that the deep learning model performance (F 1 score, precision, and sensitivity) improved with CT scan length. The X‐Net, X‐Net Ensemble, and Btrfly Net mean identification rates and localization errors were 92.4% and 2.3 mm, 94.2% and 2.2 mm, and 90.5% and 3.4 mm, respectively, in the final test set and 96.7% and 2.2 mm, 96.9% and 2.0 mm, and 94.8% and 3.3 mm, respectively, within the normative group of the final test set. The X‐Net Ensemble yielded the highest percentage of patients (94%) having all vertebral bodies identified correctly in the final test set when the three most inferior and superior vertebral bodies were excluded from the CT scan. The method used to detect labeling failures had 67% sensitivity and 95% specificity when combined with the X‐Net Ensemble and flagged five of six patients with atypical vertebral counts (additional thoracic (T13), additional lumbar (L6) or only four lumbar vertebrae). Mean identification rate on the MICCAI 2014 dataset using an X‐Net Ensemble was increased from 86.8% to 91.3% through the use of transfer learning and obtained state‐of‐the‐art results for various regions of the spine. Conclusions We trained X‐Net, our unique convolutional neural network, to automatically label vertebral levels from S2 to C1 on palliative radiotherapy CT images and found that an ensemble of X‐Net models had high vertebral body identification rate (94.2%) and small localization errors (2.2 ± 1.8 mm). In addition, our transfer learning approach achieved state‐of‐the‐art results on a well‐known benchmark dataset with high identification rate (91.3%) and low localization error (3.3 mm ± 2.7 mm). When we pre‐screened radiotherapy CT images for the presence of hardware, surgical implants, or other anatomic abnormalities prior to the use of X‐Net, it labeled the spine correctly in more than 97% of patients and 94% of patients when scans were not prescreened. Automatically generated labels are robust to widespread vertebral metastases and surgical implants and our method to detect labeling failures based on neighborhood intervertebral spacing can reliably identify patients with an additional lumbar or thoracic vertebral body.
    Type of Medium: Online Resource
    ISSN: 0094-2405 , 2473-4209
    URL: Issue
    Language: English
    Publisher: Wiley
    Publication Date: 2020
    detail.hit.zdb_id: 1466421-5
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  • 6
    In: Medical Physics, Wiley, Vol. 44, No. 11 ( 2017-11), p. 5575-5583
    Abstract: The objective of this work was to assess both the perception of failure modes in Intensity Modulated Radiation Therapy ( IMRT ) when the linac is operated at the edge of tolerances given in AAPM TG ‐40 (Kutcher et al.) and TG ‐142 (Klein et al.) as well as the application of FMEA to this specific section of the IMRT process. Methods An online survey was distributed to approximately 2000 physicists worldwide that participate in quality services provided by the Imaging and Radiation Oncology Core ‐ Houston ( IROC ‐H). The survey briefly described eleven different failure modes covered by basic quality assurance in step‐and‐shoot IMRT at or near TG ‐40 (Kutcher et al.) and TG ‐142 (Klein et al.) tolerance criteria levels. Respondents were asked to estimate the worst case scenario percent dose error that could be caused by each of these failure modes in a head and neck patient as well as the FMEA scores: Occurrence, Detectability, and Severity. Risk probability number ( RPN ) scores were calculated as the product of these scores. Demographic data were also collected. Results A total of 181 individual and three group responses were submitted. 84% were from North America. Most (76%) individual respondents performed at least 80% clinical work and 92% were nationally certified. Respondent medical physics experience ranged from 2.5 to 45 yr (average 18 yr). A total of 52% of individual respondents were at least somewhat familiar with FMEA , while 17% were not familiar. Several IMRT techniques, treatment planning systems, and linear accelerator manufacturers were represented. All failure modes received widely varying scores ranging from 1 to 10 for occurrence, at least 1–9 for detectability, and at least 1–7 for severity. Ranking failure modes by RPN scores also resulted in large variability, with each failure mode being ranked both most risky (1st) and least risky (11th) by different respondents. On average MLC modeling had the highest RPN scores. Individual estimated percent dose errors and severity scores positively correlated ( P 〈 0.01) for each FM as expected. No universal correlations were found between the demographic information collected and scoring, percent dose errors or ranking. Conclusions Failure modes investigated overall were evaluated as low to medium risk, with average RPN s less than 110. The ranking of 11 failure modes was not agreed upon by the community. Large variability in FMEA scoring may be caused by individual interpretation and/or experience, reflecting the subjective nature of the FMEA tool.
    Type of Medium: Online Resource
    ISSN: 0094-2405 , 2473-4209
    URL: Issue
    Language: English
    Publisher: Wiley
    Publication Date: 2017
    detail.hit.zdb_id: 1466421-5
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  • 7
    Online Resource
    Online Resource
    Wiley ; 2018
    In:  Journal of Applied Clinical Medical Physics Vol. 19, No. 3 ( 2018-05), p. 52-57
    In: Journal of Applied Clinical Medical Physics, Wiley, Vol. 19, No. 3 ( 2018-05), p. 52-57
    Abstract: The aim of this study was to measure and compare the mega‐voltage imaging dose from the Halcyon medical linear accelerator (Varian Medical Systems) with measured imaging doses with the dose calculated by Eclipse treatment planning system. Methods An anthropomorphic thorax phantom was imaged using all imaging techniques available with the Halcyon linac — MV cone‐beam computed tomography ( MV ‐ CBCT ) and orthogonal anterior‐posterior/lateral pairs ( MV ‐ MV ), both with high‐quality and low‐dose modes. In total, 54 imaging technique, isocenter position, and field size combinations were evaluated. The imaging doses delivered to 11 points in the phantom (in‐target and extra‐target) were measured using an ion chamber, and compared with the imaging doses calculated using Eclipse. Results For high‐quality MV ‐ MV mode, the mean extra‐target doses delivered to the heart, left lung, right lung and spine were 1.18, 1.64, 0.80, and 1.11 cG y per fraction, respectively. The corresponding mean in‐target doses were 3.36, 3.72, 2.61, and 2.69 cG y per fraction, respectively. For MV ‐ MV technique, the extra‐target imaging dose had greater variation and dependency on imaging field size than did the in‐target dose. Compared to MV ‐ MV technique, the imaging dose from MV ‐ CBCT was less sensitive to the location of the organ relative to the treatment field. For high‐quality MV ‐ CBCT mode, the mean imaging doses to the heart, left lung, right lung, and spine were 8.45, 7.16, 7.19, and 6.51 cG y per fraction, respectively. For both MV ‐ MV and MV ‐ CBCT techniques, the low‐dose mode resulted in an imaging dose about half of that in high‐quality mode. Conclusion The in‐target doses due to MV imaging using the Halcyon ranged from 0.59 to 9.75 cG y, depending on the choice of imaging technique. Extra‐target doses from MV ‐ MV technique ranged from 0 to 2.54 cG y. The MV imaging dose was accurately calculated by Eclipse, with maximum differences less than 0.5% of a typical treatment dose (assuming a 60 Gy prescription). Therefore, the cumulative imaging and treatment plan dose distribution can be expected to accurately reflect the actual dose.
    Type of Medium: Online Resource
    ISSN: 1526-9914 , 1526-9914
    URL: Issue
    Language: English
    Publisher: Wiley
    Publication Date: 2018
    detail.hit.zdb_id: 2010347-5
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  • 8
    In: Medical Physics, Wiley, Vol. 45, No. 2 ( 2018-02), p. 767-772
    Abstract: To develop a practical approach for accurate contour deformation when deformable image registration ( DIR ) is used for atlas‐based segmentation or contour propagation in image‐guided radiotherapy. Methods We developed a contour deformation approach based on 3D mesh operations. The 2D contours represented by a series of points in each slice were first converted to a 3D triangular mesh, which was deformed by the deformation vectors resulting from DIR . A set of parallel 2D planes then cut through the deformed 3D mesh, generating unordered points and line segments, to be reorganized into a set of 2D contour points. The reorganization problem was equivalent to solving the “Chinese postman problem” ( CPP ) by traversing a graph built from the unordered points with the least cost. Alternatively, deformation could be applied to a binary image converted from the original contours. The deformed binary image was then converted back into contours at the CT slice locations. We validated the mesh‐based contour deformation approach using lung and heart contours from 10 patients with thoracic cancer. Results DIR could change the 3D mesh considerably, complicating 2D contour representations after deformation. CPP could effectively reorganize the points in 2D planes regardless of how complicated the 2D contours were. Among the 10 patients, the Dice similarity coefficient between the mesh‐based contour and binary image‐based contour was 97.6% ± 0.3% for lung and 97.5% ± 0.7% for heart, and the Hausdoroff distance between them was 19.8 ± 5.1 mm for lung and 6.1 ± 2.2 mm for heart. Subjective evaluation showed that the mesh‐based approach could keep fine details, especially for the lung. The image‐based approach seemed to overprocess contours and suffered from image resolution limits. Conclusion We developed a practical approach for accurate contour deformation and demonstrated its effectiveness for both clinical and research applications.
    Type of Medium: Online Resource
    ISSN: 0094-2405 , 2473-4209
    URL: Issue
    Language: English
    Publisher: Wiley
    Publication Date: 2018
    detail.hit.zdb_id: 1466421-5
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  • 9
    In: Journal of Applied Clinical Medical Physics, Wiley, Vol. 20, No. 8 ( 2019-08), p. 47-55
    Abstract: The purpose of this study is to investigate the dosimetric impact of multi‐leaf collimator (MLC) positioning errors on a Varian Halcyon for both random and systematic errors, and to evaluate the effectiveness of portal dosimetry quality assurance in catching clinically significant changes caused by these errors. Both random and systematic errors were purposely added to 11 physician‐approved head and neck volumetric modulated arc therapy (VMAT) treatment plans, yielding a total of 99 unique plans. Plans were then delivered on a preclinical Varian Halcyon linear accelerator and the fluence was captured by an opposed portal dosimeter. When comparing dose–volume histogram (DVH) values of plans with introduced MLC errors to known good plans, clinically significant changes to target structures quickly emerged for plans with systematic errors, while random errors caused less change. For both error types, the magnitude of clinically significant changes increased as error size increased. Portal dosimetry was able to detect all systematic errors, while random errors of ±5 mm or less were unlikely to be detected. Best detection of clinically significant errors, while minimizing false positives, was achieved by following the recommendations of AAPM TG‐218. Furthermore, high‐ to moderate correlation was found between dose DVH metrics for normal tissues surrounding the target and portal dosimetry pass rates. Therefore, it may be concluded that portal dosimetry on the Halcyon is robust enough to detect errors in MLC positioning before they introduce clinically significant changes to VMAT treatment plans.
    Type of Medium: Online Resource
    ISSN: 1526-9914 , 1526-9914
    URL: Issue
    Language: English
    Publisher: Wiley
    Publication Date: 2019
    detail.hit.zdb_id: 2010347-5
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  • 10
    In: Journal of Applied Clinical Medical Physics, Wiley, Vol. 22, No. 7 ( 2021-07), p. 121-127
    Abstract: Establish and compare two metrics for monitoring beam energy changes in the Halcyon platform and evaluate the accuracy of these metrics across multiple Halcyon linacs. Method The first energy metric is derived from the diagonal normalized flatness (F DN ), which is defined as the ratio of the average measurements at a fixed off‐axis equal distance along the open profiles in two diagonals to the measurement at the central axis with an ionization chamber array (ICA). The second energy metric comes from the area ratio (AR) of the quad wedge (QW) profiles measured with the QW on the top of the ICA. Beam energy is changed by adjusting the magnetron current in a non‐clinical Halcyon. With D 10cm measured in water at each beam energy, the relationships between F DN or AR energy metrics to D 10cm in water is established with linear regression across six energy settings. The coefficients from these regressions allow D 10cm (F DN ) calculation from F DN using open profiles and D 10cm (QW) calculation from AR using QW profiles. Results Five Halcyon linacs from five institutions were used to evaluate the accuracy of the D 10cm (F DN ) and the D 10cm (QW) energy metrics by comparing to the D 10cm values computed from the treatment planning system (TPS) and D 10cm measured in water. For the five linacs, the D 10cm (F DN ) reported by the ICA based on F DN from open profiles agreed with that calculated by TPS within –0.29 ± 0.23% and 0.61% maximum discrepancy; the D 10cm (QW) reported by the QW profiles agreed with that calculated by TPS within –0.82 ± 1.27% and –2.43% maximum discrepancy. Conclusion The F DN ‐based energy metric D 10cm (F DN ) can be used for acceptance testing of beam energy, and also for the verification of energy in periodic quality assurance (QA) processes.
    Type of Medium: Online Resource
    ISSN: 1526-9914 , 1526-9914
    URL: Issue
    Language: English
    Publisher: Wiley
    Publication Date: 2021
    detail.hit.zdb_id: 2010347-5
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